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First, we have to find out what the term electrostatic actually means, so here are again our Maxwell's



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equations from the previous section.



3

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So there were four of these equations and two of them were related to the electric field and the other



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two were related to the magnetic field.



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And so, as you may expect already, by the term electrostatic, we are here only concerned with the



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electric fields.



7

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And furthermore, since the term includes static's, it means that our fields E and B, our time independent.



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So this means that this term here, the partial derivative of the magnetic field with respect to time



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is equal to zero.



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So this means here we only consider with these two equations here that the divergence of the electric



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field is basically given by the charged density, which which is position dependent.



12

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So it could be zero of our.



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And the other equation would be that the rotation of E is zero.



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And then, of course, according to these differential formulations of these two equations, we can



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also express here the integral formulations.



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So the first one looks as before and the second one is here, zero on the right side, because this



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time derivative of the magnetic field is zero.